|Publication number||US7498656 B2|
|Application number||US 10/813,886|
|Publication date||Mar 3, 2009|
|Filing date||Mar 31, 2004|
|Priority date||Oct 15, 2002|
|Also published as||US7141883, US20040178472, US20040222478, US20040222506, WO2004036654A2, WO2004036654A3|
|Publication number||10813886, 813886, US 7498656 B2, US 7498656B2, US-B2-7498656, US7498656 B2, US7498656B2|
|Inventors||Ligang Zhang, David Pietruszynski, Axel Thomsen, Kevin G. Smith|
|Original Assignee||Silicon Laboratories Inc.|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (43), Non-Patent Citations (14), Referenced by (9), Classifications (23), Legal Events (2)|
|External Links: USPTO, USPTO Assignment, Espacenet|
1. Field of the Invention
The present invention relates to integrated circuits, and more particularly to such integrated circuits incorporating shielded inductor structures.
2. Description of the Related Art
Many modern integrated circuit devices, e.g., stable oscillators, require a high-Q (i.e., quality factor) inductor that is immune to external noise sources to achieve desired specifications. Crystal oscillators may be employed, but typically require an off-chip crystal mounted elsewhere on a printed-wiring-board. LC oscillators offer the potential advantage of being able to incorporate such an oscillator on-chip.
To achieve a suitable oscillator for certain applications (e.g, inclusion in a narrow bandwidth phase-locked loop (PLL)), a high-Q (i.e., quality factor) LC oscillator is typically required. For example, a Q>20 may be required for certain applications. It is difficult to achieve such a high-Q with conventional on-chip inductors using conductor and dielectric layer compositions and thicknesses which are typically encountered in traditional integrated circuit processes. In addition, such inductors are susceptible to electromagnetic interference from external sources of noise. For certain applications using LC oscillators, a low bandwidth PLL is desirable to ensure that jitter from a noisy source is not passed to the output. In contrast, high bandwidth PLLs tend to pass input jitter. However, the ability of a PLL to resist the pulling from external noise sources is directly proportional to the loop bandwidth. Inductors inside of the PLL, particularly inside an LC oscillator included in the PLL, are most prone to pulling. Accordingly, it is desirable to shield the inductor from external noise sources, particularly in low bandwidth applications to reduce the possible degradation in performance. Therefore, improvements to high-Q LC oscillators are desired to achieve stable oscillators, particularly for use as low-jitter clock sources.
An improved electromagnetic shielding structure has been discovered. In one embodiment of the invention, an apparatus includes an inductor and an electrically conductive enclosure that electromagnetically shields the inductor. The electrically conductive enclosure has an aperture at least as large as the inductor. The aperture is substantially centered around a projected surface of the inductor. The apparatus may include one or more electrically conductive links extending across the aperture and electrically coupled to the electrically conductive enclosure. The electrically conductive links reduce an effect of electromagnetic signals external to the electrically conductive enclosure on the inductor.
In one embodiment of the present invention, a method includes reducing a current induced in an electrically conductive enclosure generated in response to an inductor. The induced current generates an electromagnetic field that counteracts an effective electromagnetic field generated by the inductor. The reducing uses at least one aperture in the electrically conductive enclosure. The method may include reducing an effective aperture utilizing links for generating a current that produces an electromagnetic field to counteract at least some external electromagnetic signals entering the electrically conductive enclosure through the aperture.
In one embodiment of the present invention, a method of manufacturing an integrated circuit product includes forming an inductor and forming an electrically conductive enclosure electromagnetically shielding the inductor. The electrically conductive enclosure has an aperture at least as large as the inductor. The aperture is substantially centered around a projected surface of the inductor. The method may include forming one or more electrically conductive links extending across the aperture and electrically coupled to the electrically conductive enclosure. The electrically conductive links reduce an effect of electromagnetic signals external to the electrically conductive enclosure on the inductor.
The present invention may be better understood, and its numerous objects, features, and advantages made apparent to those skilled in the art by referencing the accompanying drawings.
5A is a cross-sectional view of an inductor structure within an electromagnetic shielding structure in accordance with an embodiment of the present invention.
The use of the same reference symbols in different drawings indicates similar or identical items.
Another technique for reducing interference that is coupled into a resonant circuit includes shielding the inductor from outside sources of interference. A closed conducting container that reduces the electromagnetic field inside the container generated by external static electromagnetic fields forms a Faraday shield (i.e., Faraday cage) that sufficiently shields the inductor from sources of interference. A typical shielding structure includes a 6-sided electrically-conductive box (e.g., box 233 of
In response to the electromagnetic field generated by the inductor, the electrically conductive enclosure generates a current (e.g., an eddy current in a top plate, a bottom plate or sidewall of the electrically conductive enclosure) that generates a corresponding electromagnetic field that counteracts the inductor electromagnetic field. The induced current and the induced electromagnetic field are inversely proportional to a function of the distance between the inductor and a plate of the electrically conductive enclosure. The current consumes power that would otherwise be available to the inductor. The induced electromagnetic field reduces the electromagnetic field generated by the inductor. These two effects combined reduce the Q of an LC oscillator including the inductor. The plates of the electrically conductive enclosure (i.e., the top plate, bottom plate, and sidewalls) may be sufficiently spaced from the inductor to reduce the current induced in the plates of the cage. The Faraday cage is grounded at only one point to prevent DC current flow in the Faraday cage.
In an exemplary embodiment, a two-loop inductor structure of the LC tank circuit is fabricated as a shielded inductor structure. To provide adequate electromagnetic shielding, conductors used to form the shield structure should be much thicker than the skin depth (δ) corresponding to the target frequency, and the conductors should be of high conductivity to reduce eddy current losses (e.g., shield power consumption and reduction in inductor flux). Referring to
The redistribution layers are typically formed above a passivation layer, i.e., a layer formed on an integrated circuit to provide electrical stability by protecting the integrated circuit from moisture, contamination particles, and mechanical damage. The passivation layer may include silicon dioxide, silicon nitride, polyimide, or other suitable passivation materials. Redistribution layers are typically formed above integrated circuit bonding pads. These pads, typically coupled to an electronic device formed in the integrated circuit, may include aluminum, copper, titanium, or other suitable material. However, redistribution layers may include additional dielectric and conductive layers formed on an integrated circuit die in the absence of a passivation layer or bonding pads.
Redistribution layers typically have thicknesses substantially greater than the thicknesses of typical dielectric and conductive layers formed on an integrated circuit die. For example, a typical conductive layer in an integrated circuit is less than 1 μm thick and corresponding dielectric layers are also less than 1 μm thick. However, conductive layers in an exemplary redistribution layer are at least 2 μm thick and corresponding dielectric layers are at least 5 μm thick. In another embodiment, the dielectric layers are at least 15 μm thick. Redistribution dielectric layers may include silicon nitride, oxynitride, silicon oxide, benzocyclobutene (BCB), polyimide, or other suitable materials. Redistribution conductive layers may include aluminum, copper, or other suitable materials.
In an exemplary embodiment, Faraday cage 233 includes a solid top plate 230, formed in a conductive redistribution layer. Top plate 230 may be formed from a redistribution conductor layer (e.g., copper or aluminum) or under bump metallurgy. Under bump metallurgy typically provides a connection between a solder bump and a contact pad and provides a surface to which solder will adhere. The under bump metallurgy may include titanium, copper, nickel, gold, chromium and/or other suitable materials.
The bottom plate of Faraday cage 233 (i.e., bottom plate 228) is generally formed in a conductor of the integrated circuit die, i.e., a traditional integrated circuit layer or, preferably, in another conductive redistribution layer. In an exemplary embodiment, the bottom plate is formed in the first metal layer of the process technology (e.g., metal-1). However, the bottom plate may be formed in any other suitable conductive layer formed on the integrated circuit die (e.g., a traditional integrated circuit layer or a redistribution layer).
The four sidewalls of Faraday cage 233 (e.g., sidewall 220 and sidewall 222) are formed on the integrated circuit die, at least partially in redistribution layers. The sidewalls of an exemplary Faraday cage are formed partially in the typical integrated circuit layers and partially in the redistribution layers, approximated by a plurality of conductive via structures. In a typical integrated circuit process, metal layers are electrically coupled to adjacent metal layers (e.g., metal-1 is coupled to metal-2) by vias in a dielectric layer between the metal layers. Those vias are filled with conductive material.
In an exemplary embodiment, rows of vias in the typical integrated circuit layers are electrically coupled to via structures formed in redistribution layers. The via structures in the redistribution layers may be spaced a minimum distance apart and placed around the perimeter of the box, as illustrated in
In an exemplary embodiment, rows of vias in the typical integrated circuit layers, e.g., rows 554 and 552, are electrically coupled to sidewalls formed in a structure formed of under bump metallurgy (e.g., sidewalls 504 and 548). These sidewalls are formed by a non-planar layer of under bump metallurgy (e.g., the non-planar layer including top-plate 502 and sidewalls 504 and 548) that is supported by via structures e.g., support structures 556 and 550, formed in the redistribution layers. The sidewalls are coupled to portions of the Faraday cage formed in the typical integrated circuit layers, e.g., by coupling metal layer 534 in the redistribution process to metal layer 538 in the typical integrated circuit process with conductive via 536.
An exemplary Faraday cage measures 120 μm from sidewall to sidewall, surrounding a 100 pH inductor. The distance of the shielding structure from the inductor affects the resulting inductance and inductor Q. The smaller the distance, the smaller the effective inductance and the greater the loss. Typically, the sidewalls are easily positioned far enough from the inductor to reduce the effect of the sidewalls on the inductance and the inductor Q to achieve an acceptable Q. In an exemplary embodiment, the distance is approximately half the diameter of the inductor loop. In general, the inductor Q decreases at a faster rate than the inductance with decreases in distance. Forming the inductor at least partially in redistribution layers may be beneficial because the dielectric and metal layers are thicker than traditional integrated circuit layers, which facilitates achieving a sufficient distance between the inductor and the top and bottom plates of the shielding structure.
The inductor structure may be formed entirely or partially within the traditional integrated circuit layers. However, in an exemplary embodiment of the present invention, an improved Q may be achieved by forming the inductor in redistribution layers formed on the integrated circuit die, as illustrated in
An exemplary inductor includes two turns per loop, although an inductor including any number of turns per loop may be used. For a given inductance, an increase in the number of turns better confines an electromagnetic field produced by the loop because the physical size of the inductor is smaller, thus reducing the likelihood of interference from external electromagnetic fields. Concentrating the electromagnetic field generated by the inductor close to the inductor reduces distances between the top and bottom plate of the Faraday cage and the inductor necessary to achieve a particular Q. However, an increase in the number of turns increases the number of layers required to form the inductor on an integrated circuit die. In one embodiment of the present invention, the two inductor loops are formed in a planar configuration, i.e., the two loops are formed in corresponding layers on the integrated circuit die and the turns are formed in a vertical configuration, i.e., in multiple, distinct layers of the integrated circuit die. However, the inductor loops may be formed in other configurations, e.g., a vertical configuration, with the plates of the Faraday shield placed accordingly.
A three-dimensional view of the conductive layers of the inductor structure is illustrated in
Another exemplary inductor structure may be formed in redistribution layers, as illustrated in
In an exemplary redistribution and integrated circuit process, if the average distance of a copper top plate and a copper bottom plate from the inductor is dim, an exemplary inductor has a Q greater than d at 10 GHz. Referring back to
In another embodiment, the inductor structure may be formed in the traditional layers of the integrated circuit. For example, the inductor may be formed in the one or more top metal layers. One difficulty with placing the inductor in the traditional metal layers is that it reduces the distance to the bottom plate and therefore allows eddy currents formed in the bottom plate to have a greater detrimental influence on the Q of the inductor. In order to increase the distance, in one embodiment, ultra-thick layers may be used.
In one embodiment, the inductor structure may be formed in an ultra-thick layer on an integrated circuit die. Ultra-thick layers include additional dielectric and conductive layers formed on an integrated circuit die below any passivation layer and below any integrated circuit bonding pads, if present. However, ultra-thick layers may be formed on an integrated circuit die in the absence of a passivation layer or bonding pads. Ultra-thick layers typically have thicknesses substantially greater than the thicknesses of typical dielectric and conductive layers formed on an integrated circuit die. For example, a typical conductive layer in an integrated circuit is less than 1 μm thick. However, conductive layers in an exemplary ultra-thick layer are at least 3.3 μm thick and corresponding dielectric layers are at least 0.65 μm thick. Ultra-thick dielectric layers may include silicon nitride, oxynitride, silicon oxide, or other suitable materials. Ultra-thick conductive layers may include aluminum, copper, or other suitable materials. In one embodiment of the present invention, ultra-thick layers are separated from traditional integrated circuit layers by a transitional layer or layers that improve manufacturability. A transitional conductive layer has a thickness less than a thickness of an ultra-thick layer, but greater than a thickness of a traditional layer. Transitional layers may include a conductive layer and a dielectric layer and may be formed of any suitable material (e.g., silicon nitride, oxynitride, silicon oxide, aluminum, copper, polysilicon).
A top view of an exemplary inductor structure (i.e., the inductor structure formed by conductive traces 912 and 914) formed substantially in a single ultra-thick conductive layer is illustrated in
In response to the electromagnetic field generated by the inductor, the electrically conductive enclosure that electromagnetically shields the inductor generates a current (e.g., an eddy current in a top plate, a bottom plate or sidewall of the electrically conductive enclosure) that generates a corresponding electromagnetic field that counteracts the inductor electromagnetic field. The induced current and the induced electromagnetic field are inversely proportional to the distance between the inductor and a plate of the electrically conductive enclosure. The current consumes power that would otherwise be available to the inductor. The induced electromagnetic field reduces the electromagnetic field generated by the inductor. These two effects combined reduce the inductance and Q of an LC oscillator including the inductor. In addition to the advantage of ultra-thick layers giving more distance between the inductor and the bottom plate, the current generated in the electrically conductive enclosure in response to the inductor may be further reduced and a corresponding improvement to the Q of an LC oscillator including the inductor may be achieved by including one or more apertures (e.g., aperture 902) in one or more plates of the Faraday cage (e.g., bottom plate 901).
The aperture may be formed in a top plate, a bottom plate or sidewall of the electrically conductive enclosure according to the need for improvement in Q. In an exemplary process, the available vertical distance is limited, whereas sidewalls are more easily spaced to prevent the inductor from inducing a significant current in the sidewalls. Thus, aperture 902 is located in bottom plate 901 of the electrically conductive enclosure, although aperture positioning is not limited thereto. Bottom plate 901 is formed in a first traditional metal layer and a second traditional metal layer (e.g., metal-1 and metal-2). However, bottom plate 901 may be formed in any other traditional metal layer, an ultra-thick metal layer, a redistribution metal layer, other suitable materials, or any combination thereof. Although aperture 902 is placed below and substantially centered around an inductor formed substantially in an ultra-thick metal layer, a circuit element requiring electromagnetic shielding formed in traditional integrated circuit layers, redistribution layers, a package substrate, or any combination thereof and other suitable structures, may receive the benefits of an aperture appropriately placed in an electromagnetic shielding structure including an electrically conductive enclosure having a top plate, bottom plate, and sidewalls, or any other appropriate electromagnetic shielding structure.
Aperture 902 is substantially parallel to the current flow through inductor 912. Aperture 902 is larger than the inductor by approximately one half the diameter of the inductor and separates the inductor from the shield by approximately half of an inner diameter of the inductor, were the inductor projected into the same plane as the shield. An effective diameter, i.e., a diameter between two opposing linear surfaces of the aperture, may be determined by adding approximately an approximate inner diameter of the inductor to an approximate outer diameter of the inductor. For example, inductor 912 has two turns formed in 10 μm metal and has an inner diameter of 58 μm and an outer diameter of approximately 100 μm. An appropriate aperture diameter is approximately 160 μm.
In general, the Q of the inductor is proportional to aperture size, similar to the relationship between inductor Q and d, discussed above. As the aperture size increases from the outer diameter of the inductor, inductor Q increases. However, an increase in the aperture size decreases shielding of the inductor from external noise sources. Increases in aperture size beyond a certain size produce diminishing returns in improvements to Q and a tradeoff exists between increasing aperture size and decreasing shielding. Apertures having smaller diameters may be desirable in some applications (e.g., applications requiring less of a reduction in the current induced in the electromagnetic shield). Apertures having greater diameters may be desirable in applications where the losses in shielding are acceptable to obtain the corresponding increase in Q. In an exemplary application, the top and bottom plates of the electromagnetic shielding structure may be relatively close to the inductor (e.g., 10 μm) as compared to the physical size of the inductor (e.g., on average approximately 80 μm×80 μm) and an aperture may be included in the electromagnetic shielding structure by omitting one of the top and bottom plates, as illustrated by plate 972 of electrically conductive enclosure 970 in
Although aperture 902 in bottom shield 901 reduces current induced in bottom plate 901 in response to inductor 912, the aperture increases the susceptibility of inductor 912 to external electromagnetic signals. External electromagnetic signals may enter the aperture and ultimately interfere with inductor 912. To reduce the effects of external electromagnetic signals on inductor 912 and an LC oscillator including inductor 912, exemplary electrically conductive links (e.g., electrically conductive links 906 and 910 in
Exemplary electrically conductive links 904, 906, 908, and 910 are 5 μm wide and are formed in a first traditional metal layer and a second traditional metal layer (e.g., metal-1 and metal-2), the same metal layers as bottom plate 901. Like bottom plate 901, electrically conductive links 904, 906, 908, and 910 may be formed in any other traditional metal layer, an ultra-thick metal layer, two or more sub-links, a redistribution metal layer, other suitable materials, or any combination thereof. The four electrically conductive links extend from respective segments of the aperture perimeter to opposite segments of the aperture perimeter. These links intersect at 45, 90, and 135 degree angles at their respective midpoints. However, any suitable number of links may be used, intersecting at any suitable angle. In some embodiments of the present invention, a center linking structure 966 may be included to provide a 90 degree intersection interface for sub-links of links 904, 906, 908, and 910 to prevent 45 degree intersections of links 904, 906, 908, and 910.
In general, the conductive links reduce the size of the aperture (and reduce the amount of noise that can be coupled in from the outside) while maintaining the improvement in Q resulting from the creation of the aperture. A resulting Q is a function of the width of the links. Wider links allow currents induced in response to external electromagnetic fields to flow easier and produce an improvement in shielding over narrow links. However, wider links have a greater influence on the inductor by making it easier for local eddy currents induced in response to the inductor electromagnetic field to flow. The width of the links may be selected to be wide enough for better shielding, but narrow enough to provide an acceptable Q. An appropriate link width, similar to other dimensions of the invention, is dependent upon operating frequency and size of the inductor.
An exemplary plate of the electromagnetic shield (e.g., bottom plate 1100) approximates a solid metal plate by forming a plurality of continuous conductive patterns that are substantially concentric with respect to an aperture in the plate or, in one embodiment, substantially concentric with respect to the inductor projected into the same plane as the continuous conductive patterns. Referring to
Sidewalls of the electromagnetic shield may be formed in additional metal layers (e.g., metal-2-metal-8) of continuous conductive patterns that are substantially concentric with respect to the inductor projected into the same plane as the continuous conductive patterns. In one embodiment, continuous conductive patterns formed in adjacent metal layers are staggered to overlap gaps formed in next-adjacent layers. For example, metal patterns formed in metal-2 overlap the gaps formed in metal-1 (e.g., gap 1104). Continuous conductive patterns formed in alternating layers may be aligned, e.g., continuous conductive patterns formed in metal-1 are aligned with continuous conductive patterns formed in metal-3, and continuous conductive patterns formed in metal-2 are aligned with continuous conductive patterns formed in metal-4. In one embodiment of the present invention, the continuous conductive patterns formed in a metal layer are increasingly spaced out from the inductor with increasing metal layers as the metal layers approach the plane of the inductor. A resulting shielding structure includes a bottom plate having an innermost continuous conductive pattern with a smaller diameter than the upper, innermost continuous conductive patterns, as illustrated in
The continuous conductive patterns may be based at least in part on a substantially octagonal, circular, rectangular, or other suitable shape. In an exemplary embodiment, only a portion of the octagonal patterns above intersection 1110 is formed and the portions of the octagonal patterns are substantially closed by another continuous conductive pattern formed below intersection 1110. The continuous conductive patterns may be formed in typical integrated circuit layers, ultra-thick layers, redistribution layers, or other suitable conductive layers. Dimensions may vary according to a target manufacturing process. The plate may include conductive links extending across aperture 1112 as shown (not to scale). In other embodiments of the invention, bottom plate 1100 may be formed from a substantially continuous conductive layer.
In some embodiments of the present invention, the capacitor structures of the LC tank circuit and gain stages included in the oscillator circuitry may be fabricated within traditional integrated circuit layers. In some embodiments, the capacitor structures of the LC tank circuit and/or gain stages included in the oscillator circuitry may also be included within the Faraday cage, formed under the inductor in the typical integrated circuit layers. If such circuit structures are formed under the inductor in the typical integrated circuit layers, the lowest metal layer (e.g., a metal layer designated metal-1 in an exemplary process) forms the bottom plate of the Faraday cage. The Faraday cage at least partially shields the circuit elements formed underneath the inductor. The plates of the Faraday cage may allow electrical contact to these circuit elements by including openings for electrical leads. In addition, openings in the Faraday cage may exist to accommodate structures formed in the typical integrated circuit layers, e.g., an amplifier stage that is formed beneath the inductor and coupled to the inductor.
While circuits and physical structures are generally presumed, it is well recognized that in modem semiconductor design and fabrication, physical structures and circuits may be embodied in computer readable descriptive form suitable for use in subsequent design, test or fabrication stages. Accordingly, claims directed to traditional circuits or structures may, consistent with particular language thereof, read upon computer readable encodings and representations of same, whether embodied in media or combined with suitable reader facilities to allow fabrication, test, or design refinement of the corresponding circuits and/or structures. Structures and functionality presented as discrete components in the exemplary configurations may be implemented as a combined structure or component. The invention is contemplated to include circuits, systems of circuits, related methods, and computer-readable medium encodings of such circuits, systems, and methods, all as described herein, and as defined in the appended claims. As used herein, a computer readable medium includes at least disk, tape, or other magnetic, optical, semiconductor (e.g., flash memory cards, ROM), or electronic medium and a network, wireline, wireless or other communications medium.
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|US20110108947 *||Nov 12, 2009||May 12, 2011||Guzek John S||Microelectronic device and method of manufacturing same|
|US20120241905 *||Mar 25, 2011||Sep 27, 2012||Tang William W K||Substrate isolation structure|
|U.S. Classification||257/531, 257/422, 257/E23.125, 257/685, 257/528, 257/777, 257/778, 257/E21.022, 257/E23.114, 257/686, 257/277|
|International Classification||H01F27/28, H01L23/552, H01L23/64|
|Cooperative Classification||H01L2924/15311, H01L2924/01079, H01L23/645, H01F2017/008, H01L2924/3025, H01L2224/16225, H01L23/552|
|European Classification||H01L23/552, H01L23/64L|
|Mar 31, 2004||AS||Assignment|
Owner name: SILICON LABORATORIES, INC., TEXAS
Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:ZHANG, LIGANG;PIETRUSZYNSKI, DAVID;THOMSEN, AXEL;AND OTHERS;REEL/FRAME:015174/0075
Effective date: 20040331
|Aug 8, 2012||FPAY||Fee payment|
Year of fee payment: 4